Download Neutron Filter

Neutron Filter
A Mutron III Workalike
Build a clone of the classic effect
GEO Design 117
Version 1.01d
A GEO design. Copyright 1999-2001 R.G. Keen
All trademarks are property of their respective owners.
Neutron Filter
Neutron Filter, a Mutron III Workalike
The Mutron III was an envelope-controlled filter originally made by Musi-tronics. This filter
could be set to be a low pass, high pass or band pass filter, the characteristic frequency of which
followed the instantaneous loudness (or “envelope”) of a guitar signal. This means that the tone
of a signal passed through the filter changed with the loudness of a note as it rose during the
initial attack and then decayed. For the bandpass setting, the sound is very like having a wah
pedal that automatically rocks the pedal with every note.
There are other envelope-controlled filters, but the Mutron was notable for having more
flexibility of tone and sound quality. The Neutron is designed with the same technology as the
original to allow you to get the same tone. The use of a tunable state variable filter is what makes
this possible. That concept was patented in the early 70’s; the patent has now expired, so the
concept is public domain.
The Neutron has controls for:
•
Gain - how much or little the signal is amplified through the effect
•
Peak – how resonant the filter is
•
Sweep direction – whether the filter frequency goes up or down as the note gets louder
•
Range – a coarse control of whether the filter frequency is in the top or bottom of the audio
signal range.
How it works – looking at the schematic, the Neutron is composed of six operational amplifiers.
These amplifiers implement three major functional blocks:
(1) a variable gain input amplifier (U1b), with the gain set by the “Gain” control;
(2) a “state variable” filter that actually does the filtering work, made from three amplifier
sections (U1a, U2b, and U2a); and
(3) a precision rectifier/filter (U3a and U3b) that detects the instantaneous loudness of the audio
signal and uses this to control the filter center frequency.
Taking each section separately...
(1) The input amplifier is a fairly simple inverting amplifier. The gain of U1b is determined by
R3 (120K) and by the series combination of R1 and GAIN. This resistance can be varied by the
gain control from a gain of about 40 down to an attenuation of about 1/8, suiting a large range of
guitar signals. The “bypass” signal is taken from the output of this stage as well.
Note that the “bypass” signal is inverted with respect to the input signal. This is generally
recognized as a no-no today, but that’s what the Mutron did. You will probably not have any
difficulty with this unless you split your signal into two parallel paths, one of which includes the
Neutron, and then remix the two signals. Also note that the Neutron, like the Mutron, does not do
true bypass, but instead does a buffered dry signal in the “bypass” mode. You have some options
here - you can do the non-true bypass as in the original, or use a DPDT switch to do true bypass,
or the same DPDT to do true bypass with an indicator as in the "Millenium Bypass". See
http://www.geofex.com/~keen for how to do this.
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Neutron Filter
(2) The state variable filter is an unusually flexible filter, allowing as it does simultaneous output
of high, low, and band pass outputs. The control of the filter is also simple, with the filter
frequency set by two resistors and two capacitors. In this case C6 and C8 (1.8nF, or 0.0018uF)
capacitors in the feedback path of U2b and U2a and the variable resistances in parallel with R8
and R9 for those same amplifiers determine the frequency. The “Range” switch does a rough
high/low adjustment of frequency by adding an extra 2.2nF ( or 0.0022uF, C5 and C7) capacitor
in parallel with each of the 1.8nF feedback capacitors when the range switch is in the “low”
position. The variable resistances controlled by the envelope detector then sweep the filter
frequency within the selected range. The “Peak” control adds a bit of positive feedback to the
filter to allow the filter to be “peaked” at the filter frequency. This makes the bandpass higher
gain and narrower, and also puts a sharp “peak” in the response of both the high and low pass
outputs right at the cutoff frequency.
(3) The remaining two amplifiers detect the loudness of the signal and use it to drive the variable
resistances that change the filter frequency. U3b has two diodes connected to it acts as a
precision rectifier, allowing detection of even very small signals without the loss of the forward
conduction voltage as a simple diode would do. The rectified signal is filtered into a variable DC
voltage in C9 (4.7uF envelope capacitor) and then applied to the LED driver amplifier, U3a.
This amplifier simply uses the detected envelope to drive a proportional current through the
LED(s), which control the variable resistances and change the filter frequency. The “Up/Down”
switch changes the “direction” of the envelope by changing the U3a from an inverter to a
follower and changing its DC bias level to match. The LED is driven in current mode, with the
current through it sensed by the resistor noted as "Rx*" on the schematic and parts diagram.
This resistor adjusts the amount of drive current to suit the sensitivity of the specific LED; it
must be adapted for the one you use. Start with about 560 ohms and work up until you get a
value that makes your unit have about the right amount of sweep. This should be less than 4.7K.
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Neutron Filter
I see the light - the opto-electronic module originally used in the Mutron III was unique, custom
manufactured for them. It combined a single drive LED and two LDR’s in a single light-tight
package. To the best of my knowledge, it is no longer available. However, you can get the same
result four different ways, which are shown as options on the parts placement diagram. The same
PCB layout is designed to accomodate all four ways to do the optoisolator, so select the one that
suits your needs (and suppliers!) best.
Option 1 uses two H11F3 LED/photo-FET modules; Option 2 uses a single-LED/two LDR
optoisolator similar to the original(which is also very hard to find, unfortunately); Option 3 uses
two of the single LED/LDR optoisolators like the CLM6000 or the NSL32; Option 4 uses a
single LED and two discrete LDR's mounted on a 14 pin component header, a kind of discrete
version of the original opto module.
Option 1 sidesteps the difficulties of getting an LED/LDR module by using a linear LED/photofet module. These optoisolators are easily available by mail order and work well in the circuit by
actual test. They even match one another tolerably well.
In Options 2, 3, and 4, you’re using or building a functional reproduction of the original
LED/LDR circuit. Option 2 is the simplest, an LED/dual LDR module from a Japanese supplier.
These, sadly, are only available in large quantity orders usually. You might try contacting C.J.
Landry through his web site, cjlectronics, as he had some at one time. Option 3 uses a pair of
LED/ LDR optoisolators like the VTL5C3, CLM6000, NSL32, or CLM600. These modules are
moderately less rare than the original opto module, and you may well be able to find them.
Option 4 is the simplest for most people, although it requires extra work. If you buy discrete
LDR's and a high-brightness green LED, you can mount the parts on a 14pin component header
so they connect to the right points on the PCB when the component header is soldered into the
board. You will need a component header with a top cover; these are readily available from
Mouser and other suppliers. Strictly speaking, the LDRs should be matched and track, but in
practice this seems not to make too much difference to the sound. If you'd like to match the
LDR's for optimum results, buy a few extra LDR's and measure the resistance under dim to
moderate light conditions, holding the LDR's in as nearly the same orientation as you can, and
select the LDR's with the nearest two resistances.
Power to the Package - the original Mutron III used a dual 9V battery and dual-voltage AC
power supply. The Neutron has improved on this a bit by making single battery operation
possible. The 7660 module with its accompanying three 10uF and one 100uF capacitors (C15,
16, 17 and 18) form a charge pump voltage converter. This converter uses a capacitor as a
“charge bucket” to pump 9Vcharges into a –9V supply, so one battery can supply both + and –
nine volts. The disadvantage is that the power is now coming from one battery instead of two, so
the single battery drains twice as fast. However, this does make using an external DC power
supply simple, as single voltage AC powered external supplies are very common, while bipolar
ones are not. If you use the charge pump power option, populate the 7660 and capacitors, and
insert the two jumpers leading from the charge pump circuit at the bottom of the board. If you
use a dual battery or DC supply, leave all of these parts off.
Since the charge pump converter pulls pulses of current out of the battery at about 10KHz, you
must be careful that the negative battery lead NOT be part of your signal ground; if you get the
grounding wrong, you will get a high pitched whine in your sound. To prevent this, use the
battery connections shown for the charge pump converter. In this version of the board, I have
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Neutron Filter
provided Q1 and R20. Attaching a wire to the input jack stereo lug from the pad attached to R20
will switch the power off and on through Q1. Do NOT use the old trick of using a stereo jack to
switch the (-) lead to signal ground. This will guarantee that you get whine. The board layout is
specifically designed to prevent whine from the converter from getting into the signal on the
board, but as we know, reality has a way of intruding on designs. If you have wired the battery
power correctly and still have a whine, you can insert chokes instead of the two jumpers at the
bottom of the board in the power lines. This should clear up even hard cases.
If you elect to use dual batteries or a dual AC supply, simply leave off the 7660, the associated
capacitors and the jumpers. Instead, power the effect at the pads marked (+9V), (-9V), and
(Ground). The (Ground) connection serves as a star ground, and signal ground to the controls
and jacks should be connected here as well.
Parts List and Suppliers
Designation(s) Label-Value
Q1
2N3906
U1,U2,U3
TL 072 Dual Opamp
D1,D2
1N4148 diode
C1
4.7uF Tantalum
C2
0.1uF axial ceramic
C3
10pF
C4
2.2uF
C5,C7
0.0022uF (2N2)
C6,C8
0.0018uF (1N8)
C9,C10,C11
4.7uF
C12,C13
0.1uF ceramic
C14
15uF non polar
R1
3.3K
R2,R3,R16,
120K
R17,R19
R4,R20
4.7K
R5,R11
12K
R8,R9
220K
R10,R6,R7
22K
R12,R13
1M
R14
330
R15
47K
R18
180K
R21
560
GAIN
1M Rlog **
PEAK
150K log/audio pot**
Rx
150 to 4.7K, see text
Optional Parts
U4
7660 power converter
C15,C16,C17
10uF
C18
100uF
The usual stuff you'll need...
Box
Hammond 1590DD
Range,
DPDT Toggle Sw.
Direction
Mode
3PST Rotary Sw
Bypass
SPDT or DPDT
Mouser Part Numbers
625-2N3906
29SJ250-3.3K
29SJ250-120K
Qty
1
3
2
1
1
1
1
2
2
3
2
1
1
5
29SJ250-4.7K
29SJ250-12K
29SJ250-220K
29SJ250-22K
29SJ250-1M
29SJ250-330
29SJ250-47K
29SJ250-180K
29SJ250-560
313-4000-1M
313-4000-100k
1
2
2
3
2
1
1
1
1
1
1
0.07
0.07
0.07
0.07
0.07
0.07
0.07
0.07
0.07
1.74
1.74
1.79
0.07
140-XRL-25V100
1
3
1
Digi-Key
10TC260
1
2
~$12.00
2.58
10WW033
Stomp Switch
2
1
1.54
* N/A
511-TL072ACN
333-1N914
80-T350A475K010
581-SA105E104M
581-SA102A100J
140-XLR16V2.2
581-SA101C222J
80-CK05BX182K
140-XRL16V4.7
80-C315C104M5U
140-NPAL50V15
Expected Price ea.
0.10
0.85
0.15
0.39
0.12
0.19
0.05
0.27
0.30
0.07
0.12
0.71
0.07
0.07
Single Battery Option Parts
570-ICL7660CPA
140-XRL-25V10
5
0.12
Neutron Filter
1/4” jack 1-ckt
1/4" jack 2ckt
Battery clip
Stranded wire
Mono phone jack
502-111
2
1.88
Stereo phone jack
502-112B
1
1.96
9v battery clip
12BC092
1 or 2
0.38
#22 - #24 AWG
Knobs
2
** The exact values, 150K and 1M reverse log are not readily available. The substitutes listed here will work;
however, the “Peak” range is a bit restricted and the 1M is an audio taper, so must be wired and rotated counterclockwise. You can use these values until you can locate the right ones. The 1M pot works, but simply has the
reverse rotation. You could use a dual 100K audio pot for PEAK, but wire both sections in series. This will make for
a 200K audio pot, very close to the real value.
Photocell Options Parts Lists
Option 1 Parts
Description
Mouser PN
$ ea.
Qty
U100,U101
H11F3
LED/photoFET
512-H11F3
2
1.65
Option 2 Parts
Description
Source
$ ea.
Qty
LED/dual LDR
module
0805 replacement
C.J. Landry
12.00
1
Option 3 Parts
Description
Source
$ ea.
Qty
LED/LDR opto
CLM6000,
CLM600
NSL32/32A
VTL5C3
Description
Hosfelt Electr.
4.00
2
Silonex
Newark Electr.
Mouser PN
5.00
5.00
M$
Qty
Green LED,
super bright
Light variable
resistor
Component
header with
cover, 0.41 high
604-934SGC
0.21
1
338-76C59
or 338-54C79
151-314T3
1.56
2
0.78
1
Option 4 Parts
LED
LDR/photocell
14 pin header
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Neutron Filter
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Neutron Filter
Output
Jack
Optional
Power Jack
Gain Pot
Input
Jack
HP/BP/LP
Range Switch
Peak Pot
Up/Down Switch
Printed Circuit Board
Side View
of mounting
Standoff.
Stomp Switch
Batteries
Top X-Ray View of Mounting inside a Hammond 1590DD
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